Re: Klein 2-Geometry VII
David said, looking pointedly at me,
Tim Silverman joined the team and wrote many comments, perhaps he would like to sum up his discoveries.
Er … [stands nervously at front of class]
[fiddles with papers]
[squeaky voice … ]
I think that blizzard of comments was more a sign of me getting myself oriented, spotting connections between things, and going a short way up a lot of paths, than producing technical results of any interest. Given that, I think I’ll summarise my overall impression of the directions we might go in, rather than saying too much about the ground I’ve covered so far.
One danger that we seem to have encountered is that, if we start from a beautifully symmetrical and simple Klein 1-geometry and try to categorify it, the result may be rather boring, in the sense that it won’t really introduce anything new. I think this showed up with the 2-vector spaces. It appears to me that JB and David all but cleared this out right back at the beginning of that discussion, and most of what was left was pretty much finished off by Urs.
Of course, my opinion about this may perhaps just be due to my own idiosyncratic view of what counts as boring and what as interesting …
In the course of trying to get round this, I explored a couple of different paths:
1) Looking at small, runty symmetry 2-groups instead of large, beautiful ones, or examining small, runty sub-2-groups of large beautiful 2-groups. I think (in retrospect) that this is more-or-less what I was doing in the series of posts where I looked at the 2-term chain complexes of 0-forms and 1-forms over various graphs. I think that the symmetries of the graphs induce unexpected and interesting sub-2-groups of the automorphism 2-group of the chain complex itself, along with some at least mildly interesting quotient spaces. I got a bit confused and bogged down with this, from posting too fast and thinking too slowly, but I think (or hope) there is still a lot of mileage in this approach and I want to come back to it when I have sorted out some of the sub-issues in my mind.
2) Avoiding going straight down to the skeletal 2-space. I seem to be a bit out of step with everybody else here. Of course, I don’t want to be evil (i.e. forget equivalences and only think about isomorphisms). At least, not very evil. On the other hand, I still think the process by which equivalences are carried out has the potential to be interesting in particular cases. It’s not like the difference between and a single point is of no interest whatever …
From the particularities of 2-vector spaces, I then jumped up to the general case of beautifully symmetrical 2-spaces, in particular taking 1-spaces with a transitive group action on them, and constructing internal categories in categories of these spaces. While this symmetry requirement to some extent discards the interest of going to 2-spaces (e.g. it avoids going in the orbifold/stack direction of keeping track of different kinds of points), it at least lets us get an overview of all those boringly symmetrical 2-spaces.
This ‘internal category’ approach more-or-less forces us to think about the 2-space as a groupoid, and to think about the relationship between this groupoid, and the weak quotient groupoid of the object 1-space by its automorphism group (qua 1-space).
The groupoid view places at least two phenomena in front of us: isomorphisms between different points, and automorphisms of single points. It is probably a good idea to look at these separately, at least initially, although they have a good deal in common.
I tried approaching both of these through a fibre-bundle view. We can, perhaps, think of the automorphisms of a point as forming a fibre over that point; and of the objects and morphisms in one component of a groupoid as forming a kind of categorified fibre over the component (i.e. thinking of a base space whose points are the components, with the fibres being the internal structure of the components). The most obvious odd thing (to me) about this manner of thinking is that the paths in the space are global automorphisms of the base space, rather than, e.g. smooth curves. This is of course usual for Klein geometry.
I think this bundle approach, and related approaches, are worth exploring in more depth, because they may quickly connect up to a lot of other things. Judging by other threads, they’re also, perhaps, the approaches most likely to be of interest to other participants here. But I’m kind of reluctant to do too much on this, because all those other participants know such an awful lot more about this sort of thing than I do … so anything I say is liable to sound rather babyish.
At the moment, I’m having a go at working on the problem from the opposite direction: instead of picking a 2-space and trying to understand its 2-symmetry group, its figures, and its figure-symmetry sub-2-groups, I’m trying to pick a particular, very simple, 2-group and look at its various actions, as well as generally trying to understand the structure of the 2-group as thoroughly as possible.
There seem to be a very large number of different generalisations of the concepts of ‘action’ and ‘quotient’. I want to understand these and classify them. Once I’ve done that, I think a bunch of other things will become clearer.
One other point I’d like to make is that ordinary group theory is a huge, complicated subject in its own right. It’s not surprising if the theory of 2-groups has a lot of stuff lurking below the surface which isn’t simply a straightforward generalisation of the 1-group case. There’s really a tremendous lot to discover here. I really ought to familiarise myself with the existing literature, but I’m not sure I’m even at the point where I can understand it, except maybe at a very superficial and useless level.
I very much like Dave Roberts’ idea of attacking generalisations of the subobject lattice, and looking at 2-dimension via 2-ordinals. On the other hand, I’m increasingly of the opinion that the best way to categorify incidence geometry is to creep up on it from behind, rather than coming at it head-on.
To summarise the summary:
2-symmetry 2-groups which are categorifications of symmetry groups seem to have interesting 2-subgroups which are not simply categorifications of the subgroups of the symmetry groups.
Not all spaces are skeletal, and equivalences have interest beyond their mere existence!
There are some interesting things to be said about spaces which are groupoids in two different ways.
It may be interesting to think about groupoids as fibre or 2-fibre bundles.
It may be worth picking a 2-group and understanding it in detail, looking at the ways it can act as a 2-symmetry 2-group. This should involve understanding its sub-2-group lattice, and getting a better handle on what a quotient is.
Generally, we can expect interesting 2-groups to contain a lot of stuff that goes beyond what we can understand in terms of 1-groups.
To summarise the summary of the summary
Graphs, groupoids, bundles, quotients … ohhh, it’s all hard!
n-Quotients
Turning my eyes regretfully down from the gods on the heights of Olympus, I shall continue ploughing my lonely furrow at its base.
I have been thinking about quotients recently. I think I understand some things better now, so I shall put down my observations in case they are helpful to anybody else.
Weak, firm and strict quotients
We start with a groupoid. We want to think of this as a ‘weak quotient’. This usually means the result of acting on a set with a group. For each member of the group that sends an element of the set to an element , we add one morphism However, if, instead of considering an action (functor) from a group to Set, we consider more generally a functor from a groupoid to Set, sending all objects in the groupoid to the same set in Set, then we can think of any groupoid we like as being a weak quotient.
On the other hand, we have also the “strict” quotient, which is the set that we get by setting all isomorphic objects in the groupoid equal to one another and throwing away the morphisms (except identities).
I’d like to insert an intermediate level quotient. In this, we have neither a set of morphisms between two objects (as with the weak quotient), nor a “tautology” of morphisms (i.e. only the necessary identity morphisms) as with the strict quotient, but a truth value of morphisms. That is to say, if the weak quotient has at least one morphism between two objects, the intermediate quotient has exactly one. This is nothing other than a set together with an equivalence relation on it. This is nice, since an equivalence relation is traditionally seen as the intermediate step between a group action and a partition considered as a set.
What we are doing here is taking the obvious functor from the weak quotient to the strict quotient and factorising it into a full bit and a faithful bit.
Instead of this, we can try doing the steps in a different order. Instead of first reducing a set of morphisms to just one (per pair of objects), and then identifying objects, we can instead try identifying the objects first. To do this, we need to pick a particular isomorphism between each pair of objects, and “contract it down to the identity”, dragging the two objects together into one, and forcing the other isomorphisms and automorphisms to merge in a particular way. This gives us a set of groups. We can, if we wish, then force these down into a mere set of elements by identifying all automorphisms of a given object.
The fact that we can do this, merging at the 0-morphism level while failing to do so at the 1-morphism level, makes me wonder if perhaps we should have had a preliminary stage in which we add one 2-morphism from each 1-morphism to each other 1-morphism between the same objects, and then identified 1-morphisms by contraction of the 2
categorified scalar product
I have changed my mind about the nicest way to put an inner product on the 2-space. It might be good to use categories internal to hermitean vector spaces instead of just plain vector spaces. Then a good notion of categorified inner product should be given by the internal , making contact with the way I envisioned generalized Hilbert spaces of states here.